{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.92377.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1768911"}},{"@id":"https://doi.org/10.1140/epjc/s10052-020-8001-z","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"CERN-LHC. This HEPData entry describes precision measurements of the transverse momentum $p_{ll}$ (l = e, $\\mu$) and of the angular variable $\\phi_{\\eta}^{*}$ distributions of Drell-Yan lepton pairs in a mass range of 66-116 GeV. The analysis uses data from 36.1 $fb^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\\sqrt(s)$ = 13 TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final state are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proton-proton collisions at $\\sqrt(s)$ = 7 and 8 TeV, this new measurement probes perturbative QCD at a higher centre-of-mass energy with a different composition of initial states. It reaches a precision of 0.2% for the normalized spectra at low values of $p_{ll}$. The data are compared with different QCD predictions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t1","@type":"Dataset","description":"Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t2","@type":"Dataset","description":"Overview of the detector efficiency correction factors, $C_{Z}$ , for the electron and muon channels and their systematic uncertainty contributions.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t3","@type":"Dataset","description":"Measured inclusive cross-section in the fiducial volume in the electron and muon decay channels at Born level and their combination...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t4","@type":"Dataset","description":"The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at Born level as well as...","name":"Table 4a"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t5","@type":"Dataset","description":"The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at Born level as well as...","name":"Table 4b"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t6","@type":"Dataset","description":"Results of the normalized differential cross-section $1/\\sigma_\\mathrm{fid}\\times \\mathrm{d}\\sigma_\\mathrm{fid}/\\mathrm{d}p_{T}^{ll}$ measured on born level for the $Z\\rightarrow\\mu\\mu$ decay channel. The following naming...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t7","@type":"Dataset","description":"Results of the normalized differential cross-section $1/\\sigma_\\mathrm{fid}\\times \\mathrm{d}\\sigma_\\mathrm{fid}/\\mathrm{d}\\phi_{\\eta}^{*}$ measured on born level for the $Z\\rightarrow\\mu\\mu$ decay channel. The following naming...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t8","@type":"Dataset","description":"Results of the normalized differential cross-section $1/\\sigma_\\mathrm{fid}\\times \\mathrm{d}\\sigma_\\mathrm{fid}/\\mathrm{d}p_{T}^{ll}$ measured on born level for the $Z\\rightarrow ee$ decay channel. The following...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t9","@type":"Dataset","description":"Results of the normalized differential cross-section $1/\\sigma_\\mathrm{fid} \\times \\mathrm{d}\\sigma_\\mathrm{fid}/\\mathrm{d}\\phi_{\\eta}^{*}$ measured on born level for the $Z\\rightarrow ee$ decay channel. The...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t10","@type":"Dataset","description":"Results of the normalized differential cross-section $1/\\sigma_\\mathrm{fid} \\times \\mathrm{d}\\sigma_\\mathrm{fid}/\\mathrm{d}p_{T}^{ll}$ measured on bare level for the $Z\\rightarrow\\mu\\mu$ decay channel. The following...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t11","@type":"Dataset","description":"Results of the normalized differential cross-section $1/\\sigma_\\mathrm{fid} \\times \\mathrm{d}\\sigma_\\mathrm{fid}/\\mathrm{d}\\phi_{\\eta}^{*}$ measured on bare level for the $Z\\rightarrow\\mu\\mu$ decay channel. The following...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t12","@type":"Dataset","description":"Measured combined normalized differential cross-section in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate...","name":"Table 11a"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t13","@type":"Dataset","description":"Measured combined normalized differential cross-section in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate...","name":"Table 11b"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t14","@type":"Dataset","description":"The distribution of events passing the selection requirements in the electron channel as a function of dilepton invariant mass $m_{ll}$...","name":"Tabulated Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t15","@type":"Dataset","description":"The distribution of events passing the selection requirements in the muon channel as a function of dilepton invariant mass $m_{ll}$,...","name":"Tabulated Figure 1b"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t16","@type":"Dataset","description":"The distribution of events passing the selection requirements in the electron channel as a function of lepton pseudorapidity $\\eta$, the...","name":"Tabulated Figure 1c"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t17","@type":"Dataset","description":"The distribution of events passing the selection requirements in the muon channel as a function of lepton pseudorapidity $\\eta$, the...","name":"Tabulated Figure 1d"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t18","@type":"Dataset","description":"The distribution of events passing the selection requirements in the electron channel as a function of dilepton transverse momentum. The...","name":"Tabulated Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t19","@type":"Dataset","description":"The distribution of events passing the selection requirements in the muon channel as a function of dilepton transverse momentum. The...","name":"Tabulated Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t20","@type":"Dataset","description":"The distribution of events passing the selection requirements in the electron channel as a function of $\\phi_{\\eta}^{*}$. The MC signal...","name":"Tabulated Figure 2c"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t21","@type":"Dataset","description":"The distribution of events passing the selection requirements in the muon channel as a function of $\\phi_{\\eta}^{*}$. The MC signal...","name":"Tabulated Figure 2d"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t22","@type":"Dataset","description":"The measured normalized cross section as a function of $p_{ll}$ for the electron and muon channels and the combined result...","name":"Tabulated Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t23","@type":"Dataset","description":"The measured normalized cross section as a function of $\\phi_{\\eta}^{*}$ for the electron and muon channels and the combined result...","name":"Tabulated Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t24","@type":"Dataset","description":"Comparison of the normalized $p_{ll}$ distributions predicted by different computations: Pythia8 with the AZ tune, Powheg+Pythia8 with the AZNLO tune,...","name":"Tabulated Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t25","@type":"Dataset","description":"Comparison of the normalized $\\phi_{\\eta}^{*}$ distributions predicted by different computations: Pythia8 with the AZ tune, Powheg+Pythia8 with the AZNLO tune,...","name":"Tabulated Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t26","@type":"Dataset","description":"Comparison of the normalized $p_{ll}$ distribution in the range $p_{ll}$ > 10 GeV. The Born level combined measurement is compared...","name":"Tabulated Figure 6"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t27","@type":"Dataset","description":"The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at dressed level.","name":"Table 4a (dressed)"},{"@id":"https://doi.org/10.17182/hepdata.92377.v3/t28","@type":"Dataset","description":"The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at dressed level.","name":"Table 4b (dressed)"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1768911?version=3"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/92377"}],"inLanguage":"en","name":"Measurement of the transverse momentum distribution of Drell-Yan lepton pairs in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1768911?version=3","version":3}